Orbital physics can then give rise to orbital analogue phenomena of the spin Hall and spin Edelstein effects, namely orbital Hall [1]}, [2]}, [3]} and orbital Edelstein effects [4]}, [5]}, [6]}, [7]}, with the latter leading to a current-induced orbital magnetization.
Brought into the context of non-dissipative superconducting magnetoelectric effects, so far the focus has been mostly on the spin degrees of freedom for spin-Rashba type superconductors [8]}, [9]}, [10]}, [11]}, [12]}, [13]} including the generalization to all gyrotropic crystal point groups [14]}. However, since electrons carry both spin and orbital moments, assessing the role of electrons' orbital moment in setting out the magneto-electric effects is of fundamental relevance.
